Photomediated-reversible-deactivation radical polymerisation (photo-RDRP) has a limited scope of available photocatalysts (PCs) due to multiple stringent requirements for PC properties, limiting options for performing efficient polymerisations under long wavelengths. Here we report an oxygen-mediated reductive quenching pathway (O-RQP) for photoinduced electron transfer reversible addition-fragmentation chain transfer (PET-RAFT) polymerisation. The highly efficient polymerisations that are performed in the presence of ambient air enable an expanded scope of available PCs covering a much-broadened absorption spectrum, where the oxygen tolerance of PET-RAFT allows high-quality polymerisation by preventing the existence of O2 in large amounts and efficient O-RQP is permitted due to its requirement for only catalytic amounts of O2. Initially, four different porphyrin dyes are investigated for their ability to catalyse PET-RAFT polymerisation via an oxidative quenching pathway (OQP), reductive quenching pathway (RQP) and O-RQP. Thermodynamic studies with the aid of (time-dependent) density functional theory calculations in combination with experimental studies, enable the identification of the thermodynamic constraints within the OQP, RQP and O-RQP frameworks. This knowledge enables the identification of four phthalocyanine photocatalysts, that were previously thought to be inert for PET-RAFT, to be successfully used for photopolymerisations via O-RQP. Well-controlled polymerisations displaying excellent livingness are performed at wavelengths in the red to near-infrared regions. The existence of this third pathway O-RQP provides an attractive pathway to further expand the scope of photocatalysts compatible with the PET-RAFT process and facile access to photopolymerisations under long wavelengths.
Photoredox catalysis has proven to be a powerful strategy in organic transformations1 and macromolecular syntheses2,3,4,5,6,7,8,9, especially for reversible-deactivation radical polymerisation (RDRP)10,11,12. In a photo-RDRP system5,8,12,13,14,15, a specific quenching pathway describes how the photoexcitation energy is converted to chemically activate the polymerisation through a series of single electron transfer (SET) or energy transfer reactions. Established quenching pathways in photoredox catalysis include both the oxidative quenching pathway (OQP, Fig. 1a left), which involves oxidation of an excited photocatalyst (PC) and the reductive quenching pathway (RQP, Fig. 1a, middle), which involves reduction of an excited PC1. The initiating species of the photo-RDRP process can thus be activated by the excited PC via the OQP or by the PC anion (produced by reducing the excited PC) via the RQP.
Despite the successful implementation of these pathways to regulate photo-RDRP, the scope of efficient PC candidates is however very much limited (Fig. 1a). This is primarily due to the stringent requirements for an efficient PC to serve as a sufficiently strong excited-state reductant in OQP or excited-state oxidant in RQP16. In the context of photo-RDRP, increasing catalyst versatility is vital for its successful implementation in various application scenarios and media. Furthermore, in stark contrast to thermal reactions which proceed at a single elevated temperature, the narrow absorptions of PCs extending into the visible and near-infrared (NIR) ranges can be exploited for multiple concurrent, potentially orthogonal, reactions in the same volume17,18,19,20. In particular, NIR light provides promoted light penetration and reduced side reactions as a benign light source21,22,23. Previously, we discovered that a metalloporphyrin, zinc octaethyltetraphenyl porphyrin, could not facilitate polymer synthesis via the established OQP or RQP mechanisms and only in the presence of atmospheric oxygen did the polymerisation proceed, with inert gases providing a means to temporarily pause the process. Critically, polymerisations were not observed in the absence of RAFT agent; this observation, in conjunction with the polymerisation proceeding at accelerated rates in the presence of pure oxygen, led to the hypothesis that oxygen (O2) could be playing the role of a mediator to specifically activate the RAFT agent.
In this work, experimental and computational studies are combined to clarify and validate the underlying mechanism of this pathway, which we have designated as O2-mediated RQP (O-RQP, Fig. 1a, right). From an initial group of four different PCs, varied selectivity of the quenching pathways is identified and used as the basis for discerning the thermodynamic requirements of different pathway in silico. This knowledge facilitates the identification of four other O-RQP compatible catalysts. The mechanistic pathway established herein provides an oxygen-tolerant RDRP process that is particularly efficient with PCs capable of absorbing low-energy photons, with wavelengths ranging from orange to the NIR region without activating the established OQP and RQP pathways1.
Experimental screening of PCs
Despite significant effort devoted to the discovery of PCs for PET-RAFT polymerisation via the OQP or RQP, the scope of efficient PCs available is still very limited, especially for candidates with longer-wavelength light absorption. This is primarily due to strict thermodynamic constraints of PCs in the OQP and RQP (Fig. 1). In the OQP, OQP-I is a process where 3PC* absorbs energy and donates an electron from its upper singly occupied molecular orbital (upper-SOMO). Consequently, a 3PC* with lower-lying upper-SOMO is less likely to activate OQP-I (requires more energy to donate an electron) and can thus be ineffective for the OQP. Conversely, in the RQP, RQP-I is a process where 3PC* accepts an electron (releasing energy) to its lower-SOMO leading to RQP-II where the PC•− donates that electron (absorbing energy) from its only SOMO. Hence, either a higher-lying lower-SOMO of 3PC* (releasing less energy to accept an electron) or lower-lying SOMO of PC•− (requiring more energy to donate an electron) can increase the overall energy requirements, decreasing the efficiency to which 3PC* can facilitate the RQP. Indeed, these complex thermodynamic constrains have excluded a great number of dyes from being effective or efficient for PET-RAFT polymerisation. These constraints could also be responsible for many selectivities of certain PCs with respect to specific RAFT agents24,25.
The discovery of O-RQP originates from our recent finding that suggested singlet oxygen (1O2) generated by 3PC* can react with triethylamine (TEA) to form superoxide (O2•−), which can further interact with the 3PC* and activate the chain-transfer agent (CTA)26. This deviated from the known RQP pathway in that no polymerisation was observed in the absence of oxygen, suggesting the existence of an alternative activation pathway. In following re-evaluation, we discovered that the interaction between O2•− and 3PC* is not necessary to activate the CTA, as O2•− is thermodynamically capable of directly activating trithiocarbonates (vide infra). With the onus of activation lying with superoxide, this mechanism has the potential to be generalised and expanded to encompass a much broader range of chromophores. To investigate this potential, we first compared a selection of four chromophores, two that were known to be compatible with PET-RAFT and two other candidates. First, zinc(II) 5,10,15,20-(tetraphenyl)porphyrin (ZnTPP, Fig. 2b), which has exhibited excellent efficiency towards PET-RAFT at extended wavelengths, was selected as the baseline in terms of thermodynamic characteristics associated with effective OQP catalysis. Although possessing a similar structure to that of ZnTPP, the non-metallated 5,10,15,20-(tetraphenyl)porphyrin (TPP, Fig. 2c) has exhibited significantly worse ability to regulate PET-RAFT via the OQP. Additionally, its capability to mediate PET-RAFT via the RQP has yet to be investigated and therefore provided an interesting proposition for this study. From these two known PCs, we further selected zinc(II) 2,3,7,8,12,13,17,18-octaethylporphyrin (ZnOEP, Fig. 2a) and zinc(II) 5,10,15,20-(tetra-trimethylsilylethynyl)porphyrin (ZnTSP, Fig. 2d); owing to the lack of electron-withdrawing phenyl groups, the former is likely to be a more reductive PC in comparison to ZnTPP. In contrast, the ethynyl substituents of ZnTSP leads to an expanded macrocycle and hence more stabilised (in terms of π* orbitals) species that requires lower excitation energy at the expense of weaker excited-state redox capabilities. Detailed discussions with respect to the structure–property relationships are presented in Supplementary Note 5. Although sharing structural similarities, the four PCs were predicted to present varying degrees of photocatalytic capabilities and therefore enabled the isolation of the O-RQP mechanism for more detailed investigation.
A model PET-RAFT system was used for consistency in all cases, with 2-(dodecylthiocarbonothioylthio)propionic acid (DTPA) as the chain-transfer agent (CTA), methyl acrylate (MA) as the monomer and dimethyl sulfoxide (DMSO) as the solvent (Fig. 1b) for the OQP, at a fixed molar ratio of [CTA]:[monomer]:[PC] = 200:1:0.01 and monomer to solvent 1:1 v/v (details see Supplementary Note 3). The selection of DTPA and MA as the model system was not only in consideration that they are commonly used in kinetic studies but also because the thermodynamic properties of DTPA before and after one or more MA additions are essentially the same (see Supplementary Note 3 and Supplementary Fig. 1), which is ideal for thermodynamic studies and theoretical evaluation. To enable the RQP, the model co-catalyst triethylamine (TEA, Fig. 1b) was added at 0.5 equivalence to the CTA. To enable an O-RQP, the same recipe used for RQP was sealed without deoxygenation (in the presence of air). In contrast, polymerisations via an OQP or the RQP were deoxygenated by purging with nitrogen for 10 min prior to light irradiation. Nominal wavelengths of the light source were chosen according to the red-most absorption peak (the lower energy Q-band) of the porphyrin-based molecule, i.e. 565 nm yellow light for ZnOEP, 590 nm orange light for ZnTPP, 625 nm red light for TPP, and 660 nm deep-red light for ZnTSP at 10 mW/cm2 using light-emitting diodes (LEDs, more details for consideration of selecting irradiation sources see Supplementary Note 3).
Utilising this standardised approach, the polymerisation kinetics mediated by each of the selected catalysts were investigated to ascertain differences in capabilities with respect to the three catalytic pathways (Fig. 2). Survey of the pseudo-first-order kinetic plots for each of the PCs (Fig. 2e–h) provides interesting insights into the varied capabilities of each species. Those possessing strong reducing capabilities, ZnOEP (Fig. 2e) and ZnTPP (Fig. 2f) were observed to be effective mediators of all three reaction conditions. In contrast, TPP showed limited ability to mediate PET-RAFT via the RQP and inability to facilitate the OQP in the investigated time frame. ZnTSP on the other hand was found to be effective for the oxygen-mediated pathway (O-RQP) only. In fact, with all four species demonstrating robust performance via this pathway, it leads to the suggestion that O-RQP may indeed be the “path of least resistance”. The predominant reason for the inertness of ZnTSP in OQP and RQP is the four electron-withdrawing ethynyl groups which decreases the energy of the lowest unoccupied molecular orbital (LUMO; Supplementary Fig. 34, l) compared to the other PCs. As the lower-lying LUMO corresponds to a lower-lying upper-SOMO of the excited-state PC (3PC*), the OQP is made less favourable. Additionally, the lower-lying SOMO of ZnTSP•− makes it less favourable for RQP and consequently it displayed the lowest activity among the four PCs (i.e., inert for OQP and RQP). Irrespective of the pathway in which the polymerisations proceeded, clear evidence of temporal control was demonstrated by the ability to temporarily pause the process with full recovery of the rate upon switching the light back on. Analysis by gel permeation chromatography revealed narrow molecular weights that clearly shifted towards higher molecular weight with increasing irradiation time for all cases (Supplementary Figs. 2–10; molecular weight dispersity Mw/Mn ~1.1, Fig. 2i–l). Living characteristics of a linear first-order kinetic plot (Fig. 2e–h) and linear increases in molecular weight (Mn) with increasing conversion (Fig. 2i–l) were further supported by nuclear magnetic resonance (NMR) spectroscopy (Supplementary Fig. 16) and matrix-assisted laser desorption/ionisation-time of flight (MALDI-TOF) mass spectroscopy (Supplementary Fig. 18), which confirmed high end-group fidelity of the synthesised polymers. Notably, no noticeable side effects stemming from the presence of O2 on the synthesised polymer were observed, consistent with our previous observations27,28,29. Chain extension experiments for all synthesised polymers were performed with dimethylacrylamide (DMA) to produce block copolymers; complete shifts of molecular weight distribution (MWD) towards higher molecular weights in conjunction with narrow molecular distributions (Mw/Mn ~1.1, Supplementary Figs. 19–27), lend further support to the high retention of end groups in all cases. O-RQP polymerisations performed in various solvents and for different monomers also proved to be successful, demonstrating the generality of the approach (Supplementary Fig. 41 and Supplementary Table 17). Details are presented in Supplementary Note 11.
Theoretical investigation of PCs
The use of redox potentials to explain the activation of initiators by a PC for photo-RDRP is a reasonable approach when the electrochemical properties of the investigated PCs are to be qualitatively compared in a single photo-RDRP system with a given initiator29,30,31,32. However, when examining each catalytic mechanism in greater detail, such as the thermodynamic interplay between PCs and different quenching pathways, the above methods fall short of the required quantitative accuracy. In this work, where the thermodynamic favourability of a PC in activating different quenching pathways is of interest, the calculation of the change in Gibbs free energy (ΔG) for each SET event, in conjunction with a theoretically derived activation threshold, provides a clearer picture with regard to the viability of the various SET events.
Each of the catalytic pathways are composed of steps involving both excited-state and ground-state species. Based on Marcus theory, SET reactions between excited-state species and ground-state species can usually be classified into two major types. The SET reaction between an excited-state reactant and a ground-state reactant (ES–GS SET, i.e., PET) is irreversible. On the other hand, an SET reaction between two ground-state species (GS–GS SET) is a reversible process33. For more details see Supplementary Note 8. In the case of GS–GS SET, we define ΔG as the Gibbs free energy change of an SET process (describing its favourability at a specific temperature, i.e. at room temperature here) and ΦSET,GS–GS as the quantum yield of a GS–GS SET process (expressed as Supplementary Eq. 1 in Supplementary Note 8 describing how likely the reversible GS–GS SET ends up with products after the SET event). By collectively solving equations for the ΦSET,GS–GS expression (Supplementary Eq. 1), the equilibrium constant K expression34,35,36 (Supplementary Eq. 2), the Nernst equation at equilibrium37,38 (Supplementary Eq. 4), we derived the relation between ΦSET,GS–GS and ΔG (Supplementary Eq. 5) and correspondingly derived the thermodynamic thresholds for GS–GS SET. This leads to the quantum yield of a GS–GS SET process (ΦET,GS–GS) being equal to 50% at ΔG = 0 kcal/mol, 1.45% at ΔG = 5 kcal/mol, and 0.05% at ΔG = 9 kcal/mol. Utilising the assumption that a quantum yield of less than 0.05% (ΦET,GS–GS < 0.05%) is inadequate to facilitate the generation of sufficient quantities of reactive species for the next step, provides us with a prohibitive threshold (ΔG > 9 kcal/mol) wherein the reaction is deemed unlikely to proceed. On the other hand, when ΔG < 5 kcal/mol, ΦET,GS–GS > 1.45%, and is considered to afford effective activation of the reactive step (activation threshold = ΔG < 5 kcal/mol). For more details see Supplementary Note 8.
In the case of PET (ES–GS SET), because it is known to be irreversible33, only the rate of the PET process kPET is the limiting factor for efficiency. Indeed, kPET of a specific PET process must be high enough for PET to occur within the excited-state lifetime of the photo-excited reactant, otherwise the PET process will not proceed. As Marcus theory clearly suggests that thermodynamics controls the kinetics of SET processes39,40 (based on the Arrhenius41 and Eyring42,43 equations), there must be thermodynamic thresholds for the PET process. To quantify these thresholds, we introduced the Eyring equation42,43 and established the relationship between kPET and ΔG (Supplementary Eq. 6 in Supplementary Note 8). Because the T1 lifetime of porphyrins are generally on the ms-scale, PET with a half-life t(1/2) (expressed as Supplementary Eq. 7) <10 ms (corresponding to ΔG < 15 kcal/mol by solving Supplementary Eqs. 6 and 7) can be considered efficient at room temperature (i.e. a notable number of PET events can proceed within the T1 lifetime), whereas PET with a t(1/2) > 100 ms (corresponding to ΔG > 16 kcal/mol) is assumed ineffective at room temperature. Thus, we derived ΔG < 15 kcal/mol to be considered efficient (activation threshold) and ΔG > 16 kcal/mol to be considered ineffective (prohibition threshold). More details are discussed in Supplementary Note 8. With these boundary conditions established, we performed thermodynamics calculations for all four dye-catalysed photo-RDRP systems via OQP, RQP and O-RQP, respectively, to examine the theoretically derived thresholds. By comparing the thermodynamic properties of each specific SET processes in correlation with the experimentally observed selectivity, we confirmed the viability of the derived thermodynamic thresholds in practice (vide infra).
The OQP is perhaps the simplest quenching pathway in PET-RAFT, which only requires the presence of the PC to fulfil the catalytic cycle and activate the RAFT agent (Fig. 3a). This two-step pathway is composed of a PET process (OQP-I, Fig. 3a; possibility of energy transfer is discussed in Supplementary Note 7) that is followed by a GS–GS SET deactivation step (OQP-II, Fig. 3a). The two processes have distinct differences with regard to their thermodynamic viabilities; OQP-I, as a PET step, was deemed to be efficient when ΔG < 15 kcal/mol and prohibited if ΔG exceeded 16 kcal/mol. On the other hand, OQP-II, which is a reversible GS–GS SET process composed of both forward and reverse SET reactions, can effectively proceed when ΔG is less than 5 kcal/mol and is suppressed when ΔG exceeds 9 kcal/mol. To clarify the thermodynamic viability of these steps with respect to the individual PCs, density functional theory (DFT) calculations were performed to derive the ΔG for both OQP-I (ΔGI, activation of RAFT) and OQP-II (ΔGII, deactivation of RAFT). As supported experimentally (Fig. 2e–h) and computationally (Fig. 4a–d), ZnOEP and ZnTPP are efficient PCs for OQP-I, while TPP and ZnTSP are unable to facilitate this crucial step (for consideration of exact kinetics see ref. 21). Regardless of the viability of the deactivation step (OQP-II) for all PCs investigated herein, the inability to facilitate the OQP-I step highlights the major barrier precluding many potential candidates from application in the PET-RAFT process via oxidative quenching.
The RQP incorporates a co-catalyst, in this case, TEA, to facilitate reduction of the excited PC (ES–GS SET, RQP-I, Fig. 3b). A subsequent GS–GS SET between the PC radical anion (PC•−) and the RAFT agent initiates the polymerisation process (RQP-II, Fig. 3b). Finally, the active RAFT agent (CTA•−) is deactivated into the dormant species (CTA) via a GS–GS SET (RQP-III, Fig. 3b) with the TEA radical cation (TEA•+) that was originally formed during RQP-I. For all four PCs, it appears that the thermodynamic requirements for RQP-I (3PC* reduction) and RQP-III (RAFT deactivation) are satisfied and it is the activation of the RAFT agent by the PC•− (RQP-II), which determines the success of the reaction (Fig. 4e–h). TPP, while viable in this step (ΔGII = 5 < 5.98 < 9 kcal/mol), is significantly less efficient because of its relatively low ΦET,GS–GS = 0.64%. For ZnTSP, this step is unviable, and polymerisation is therefore prohibited (ΔGII = 12.81 kcal/mol > 9 kcal/mol and ΦET, GS–GS = 0.00%), as confirmed experimentally.
By contrast, O-RQP is a less PC-dependant pathway. As shown both experimentally (Fig. 2e–h) and computationally (Fig. 4i–l), the O-RQP mechanism is a viable and effective pathway for all four PCs and leads to the suggestion that it is indeed less dependent on the redox capabilities of the PC. As revealed in the proposed mechanism (Fig. 3c), O-RQP-I, O-RQP-II and O-RQP-III are independent of the PC employed. Indeed, DFT calculations for O-RQP-I (the ES–GS SET process between 1O2 and TEA to yield O2•− and TEA•+) exhibits ΔGI = −1.14 kcal/mol < 15 kcal/mol (highly favourable). As reported26,44, O2•− was experimentally detected as the product of 1O2-TEA reaction. To verify if the 1O2-TEA reaction can substantially occur to yield O2•−, we utilised ZnTSP (inert with OQP and RQP) as the photosensitiser to generate 1O2 in the presence of the 1O2 trapper, 9,10-dimethylanthracene (DMAn) to yield an endoperoxide, under 660 nm irradiation. The decreasing peak intensities of DMAn (402 nm) with irradiation time is indicative of 1O2 generation, fulfilling the necessary first step of the proposed O-RQP mechanism (Supplementary Fig. 36, b). Addition of TEA into the same system ([PC]:[TEA] = 0.01:0.5, same as above) significantly retarded the consumption of DMAn. Further increase in the concentration of TEA ([PC]:[TEA] = 0.01:5) led to cessation of DMAn consumption (details see Supplementary Note 9). The suppression of endoperoxide formation with increasing TEA concentrations implied the competition for the same substrate (the TEA-1O2 reaction and the DMAn-1O2), with the formation of O2•− being evidently more efficient.
With the O2•−-DTPA reaction seemingly the primary activation step we probed this reaction in greater detail. We performed DFT calculations on the bimolecular system and observed strong electrostatic affinity between DTPA and O2•− as well as significant intermolecular charge transfer (CT) from O2•− to DTPA, which is favourable for the O2•−-DTPA SET to occur (Supplementary Fig. 40). On the other hand, the product DTPA•−-O2 exhibits no electrostatic affinity nor CT character, which is favourable for rapid O2 diffusion into the solution (Supplementary Fig. 40). Therefore, O-RQP-II can be considered a CT-assisted irreversible process that satisfies the activation threshold of 15 kcal/mol. Accordingly, we calculated ΔG of O-RQP-II to be 10.76 < 15 kcal/mol (Supplementary Note 10). With respect to 1O2 photosensitisation, due to the complexities regarding the generation of 1O2 (i.e. whether it exists as free 1O2 or a (PC-O2)* complex etc.)45,46, we cannot perform further computational studies at present. Indeed, this aspect has remained in debate for decades and comprehensive ES dynamics is required to resolve the issue. With the combination of theoretical and experimental results suggesting the thermodynamic favourability of O2•− generation at room temperature, it appears that the predominant role of the PC in the O-RQP process is that of a photosensitiser to generate 1O2.
As suggested by our previous contribution, the dual role of O2 as a radical scavenger and a catalytic species, is a “paradox”26. Specifically, the propagating carbon radical in a polymerisation is subject to oxidation by ground-state O2 leading to the formation of a peroxy radical47 and degradation of the dormant polymer chain may also occur in the presence of ground-state O248. However, unlike conventional, thermally initiated RAFT polymerisations, the PET-RAFT systems possess excellent oxygen tolerance as reported in previous publications, where O2 is rapidly converted to 1O2 upon irradiation and chemically quenched by the solvent DMSO, forming DMSO224,27,28,29,49,50,51. In this context, the interplay between the oxygen tolerance feature and the catalytic role of O2 in PET-RAFT polymerisation via O-RQP mechanism lies in the amount of O2; the oxygen tolerance feature facilitates high-quality polymerisation by lowering the O2 concentration to the catalytic amounts required for efficient O-RQP.
To increase the readability of the supportive discussion of the O-RQP mechanism above, which is composed of a 1O2 photosensitisation process, followed by O-RQP-I (electron transfer reaction between 1O2 and TEA), O-RQP-II (activation of RAFT by superoxide O2•−) and O-RQP-III (deactivation of RAFT) processes, we summarised the chain of evidence from both experimental and computational studies, supporting literature and comparative studies as Supplementary Fig. 46 and Supplementary Note 14.
Extension of O-RQP to phthalocyanines
Confirmation of the reduced photocatalytic requirements for conducting O-RQP opens opportunities to expand the scope of PCs suitable for PET-RAFT. However, the production of reactive oxygen species (ROS), in the form of both 1O2 and O2•−, throughout the entire polymerisation process means that dyes susceptible to ROS-induced degradation may be unsuitable for this approach. Taking this limitation into consideration, we turned our attention to phthalocyanines. Phthalocyanines, as structural cousins to porphyrins, offer significantly easier preparative routes, making them the superior economical choice for industrial implementation52,53,54. Additionally, these species offer Q-bands that extend into the far-red to NIR regions with facile modification routes to facilitate further red-shifting; the application of phthalocyanines to PET-RAFT could greatly expand the range of serviceable wavelengths23,55,56,57. However, asides from utilisation in photodynamic therapy, the photocatalytic capabilities of phthalocyanines have been limited. The discovery of O-RQP presents more promise in that activation of the CTA is governed by the interaction of O2•− with the RAFT agent; the role of the phthalocyanine is simply to produce 1O2 (refs. 55,58,59).
Starting with the azaporphyrin zinc (II) 2,7,12,17-tetra-tert-butyl-5,1-,15,20-tetraaa-porphine (ZnTtBAzP), which possesses structural similarities with phthalocyanines but with unsaturated β-pyrrole positions, we sought PCs with increasingly red-shifted Q-bands. To this end, zinc (II) 2,9,16,23-tetra-tert-butyl-phthalocyanine (ZnTtBPC), zinc (II) 1,4,8,11,15,18,22,25-octabutoxy-phthalocyanine (ZnOBOPC) and zinc (II) 2,11,20,29-tetra-tert-butyl-2,3-napthalocyanine (ZnTtBNPC) were selected for their application in O-RQP PET-RAFT. For spectral details see Supplementary Note 5. Experimental screening (0% monomer conversion in 2 h) showed that these PCs were inert for both the OQP and RQP as expected. Thermodynamic studies (Table 1) further highlighted their difficulties with regard to the respective pathways. Interestingly, with all four dyes were calculated to be inert for RQP; ZnTtBAzP and ZnTtBPC were ineffective for RQP-II whereas ZnOBOPC was ineffective for RQP-I and ZnTtBNPC ineffective for both steps. More detailed discussions are presented in Supplementary Note 6.
Despite their inability to facilitate the OQP or RQP PET-RAFT polymerisations, these selected examples were highly effective in promoting the O-RQP process under irradiation wavelengths ranging from 590 to 780 nm (Fig. 5). In line with the results obtained for ZnTSP, the polymerisations performed using these dyes exhibited living controlled characteristics, such as a linear first-order plot, wherein the interruption to the irradiation caused negligible impact on the recovery of the polymerisation rate upon resumption. Additionally, molecular weights increased linearly with increasing conversion and were concomitant with narrowing of the MWDs (Supplementary Figs. 11–15). End-group retention was confirmed by chain extensions, which resulted in complete shift of the MWDs towards higher molecular weights (Supplementary Figs. 28–32).
Overall, through an approach combining experimental studies and computational investigation, the mechanism of an oxygen-mediated reductive quenching catalytic pathway (O-RQP) was presented, which eliminates sufficient O2 to the point where radical polymerisation proceeds unencumbered while the remaining catalytic amounts of O2 serve as a co-catalyst to provide facile polymerisation. Critically, (TD-)DFT calculations provided guidelines highlighting the thermodynamic favourability of a PC for a given catalytic pathway. Among these, O-RQP only necessitates the PC to be capable of generating singlet oxygen (1O2). To demonstrate the lowered requirements for O-RQP, we investigated four phthalocyanine derivatives, which have seen limited use in a photocatalytic context, in their ability to catalyse PET-RAFT polymerisation. While their implementation in OQP and RQP modes failed to yield any polymers, they were highly successful within the O-RQP framework. Exploiting the extended Q-bands of these phthalocyanines, well-controlled polymerisations exhibiting excellent livingness were performed in the presence of oxygen. The existence of the O-RQP mechanism provides an accessible avenue to increasing the scope of PCs that can enable better usage of a wider electromagnetic spectrum, especially long wavelengths in the NIR range.
General procedures for computation
Geometry optimisations for PCs (and other species) were performed at the B3LYP-GD3BJ/6-311G* level of theory (pseudopotential basis set LanL2TZ for zinc; SMD-DMSO solvation model), with the Gaussian09 D01 software package60 installed in the Katana high-performance computing clusters at the University of New South Wales. The T1 states were calculated by UDFT. Single-point energy calculations were further performed at the B3LYP-GD3BJ/6-311+G** level of theory for both ground states and T1 states (UDFT). More details see Supplementary Note 13.
General procedures for thermodynamic studies
To evaluate the thermodynamics of each electron transfer catalytic process, the Gibbs free energy change (ΔG) was calculated as ΔG = G(P1) + G(P2) − G(R1) – G(R2), where G(P1) and G(P2) represent the Gibbs free energies (G) of products while G(R1) and G(R2) represent those of reactants. G of each species was taken as the electronic energy as common practice, since this is sufficiently accurate for thermodynamic studies of electron transfer events.
The authors declare that the data supporting the findings of this study are available within the paper and its Supplementary Information.
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C.B. acknowledges the Australian Research Council (ARC) for his Future Fellowship (FT120100096) and discovery project (DP180102540 and DP190100067). W.L. acknowledges National Natural Science Foundation of China (Grant Nos. 21973054 and 21833001).
The authors declare no competing interests
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Wu, C., Jung, K., Ma, Y. et al. Unravelling an oxygen-mediated reductive quenching pathway for photopolymerisation under long wavelengths. Nat Commun 12, 478 (2021). https://doi.org/10.1038/s41467-020-20640-z